# Interaction of Hadronic Dark Matter with Nucleons and Leptons

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## Abstract

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## 1. Introduction

## 2. Meson-Exchange Model of New Hadrons Interaction with Nucleons

- Octet of baryons $B=(N,\Theta ,\Sigma ,{\Lambda}^{0})$ (adjoint representation of strong group $SU(3))$.
- Singlet ${V}^{0}$ and octet $V=(\rho ,{\varphi}^{0},{K}^{*},{\overline{K}}^{*})$ of vector mesons (gauge fields).
- Three triplets of scalar mesons $H=({a}_{0},{f}_{0},{f}_{0}^{{}^{\prime}},{K}_{0},{\overline{K}}_{0})$ (higgs fields).
- Octet of pseudoscalar fields $\Phi =(\pi ,\eta ,K,\overline{K})$ (adjoint representation).

## 3. Cross-section of Nucleons Scattering on New Hadrons

## 4. Interaction of New Hadrons with Leptons

## 5. Conclusions

## Author Contributions

## Funding

## Acknowledgments

## Conflicts of Interest

## References

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**MDPI and ACS Style**

Beylin, V.; Kuksa, V.
Interaction of Hadronic Dark Matter with Nucleons and Leptons. *Symmetry* **2020**, *12*, 567.
https://doi.org/10.3390/sym12040567

**AMA Style**

Beylin V, Kuksa V.
Interaction of Hadronic Dark Matter with Nucleons and Leptons. *Symmetry*. 2020; 12(4):567.
https://doi.org/10.3390/sym12040567

**Chicago/Turabian Style**

Beylin, Vitaly, and Vladimir Kuksa.
2020. "Interaction of Hadronic Dark Matter with Nucleons and Leptons" *Symmetry* 12, no. 4: 567.
https://doi.org/10.3390/sym12040567